JPH0422456B2 - - Google Patents

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Publication number
JPH0422456B2
JPH0422456B2 JP59236928A JP23692884A JPH0422456B2 JP H0422456 B2 JPH0422456 B2 JP H0422456B2 JP 59236928 A JP59236928 A JP 59236928A JP 23692884 A JP23692884 A JP 23692884A JP H0422456 B2 JPH0422456 B2 JP H0422456B2
Authority
JP
Japan
Prior art keywords
deterioration
power spectrum
deterioration index
abnormality
vibration
Prior art date
Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
Expired - Lifetime
Application number
JP59236928A
Other languages
Japanese (ja)
Other versions
JPS61114134A (en
Inventor
Satoshi Ueda
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
Nippon Steel Corp
Original Assignee
Sumitomo Metal Industries Ltd
Priority date (The priority date is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the date listed.)
Filing date
Publication date
Application filed by Sumitomo Metal Industries Ltd filed Critical Sumitomo Metal Industries Ltd
Priority to JP59236928A priority Critical patent/JPS61114134A/en
Publication of JPS61114134A publication Critical patent/JPS61114134A/en
Publication of JPH0422456B2 publication Critical patent/JPH0422456B2/ja
Granted legal-status Critical Current

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Classifications

    • GPHYSICS
    • G01MEASURING; TESTING
    • G01HMEASUREMENT OF MECHANICAL VIBRATIONS OR ULTRASONIC, SONIC OR INFRASONIC WAVES
    • G01H1/00Measuring characteristics of vibrations in solids by using direct conduction to the detector
    • G01H1/003Measuring characteristics of vibrations in solids by using direct conduction to the detector of rotating machines

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  • Physics & Mathematics (AREA)
  • General Physics & Mathematics (AREA)
  • Testing Of Devices, Machine Parts, Or Other Structures Thereof (AREA)
  • Measurement Of Mechanical Vibrations Or Ultrasonic Waves (AREA)

Description

【発明の詳細な説明】[Detailed description of the invention]

〔産業上の利用分野〕 本発明は、減速機、モータ、ブロワ等の回転機
械、或いは軸受、歯車等の回転機械要素における
異常状態の診断方法に関する。 〔従来技術〕 モータ、ブロワ等の回転機械、或いは転がり軸
受、歯車等の回転機械要素においては、回転によ
る摩耗、損傷、或いは潤滑不良による損傷、また
は組付け不良による損傷等が生じる。このため、
回転機械等に生じる損傷等を早期に発見して対処
する必要が生じる。 回転機械等の異常の診断方法としては、摩耗、
損傷等の異常に起因して生じる振動を捉える振動
法が一般的である。従来の振動法は、回転機械等
の振動を測定し、その振動を高速フーリエ変換す
ることにより、時間領域で表わた不規則関数であ
る振動を、周波数領域の関数に変換して、そのパ
ワースペクトルを求め、求められたパワースペク
トルから劣化指数を算出して、回転機械等の異常
状態を判断するものであつた。 〔発明が解決しようとする問題点〕 回転機械等における振動は、摩耗、損傷等の異
常に起因する振動以外の振動(ノイズ)、特に一
過性のものが含まれているため、従来の振動法で
はこれらのノイズを完全に除去できず、正確な劣
化指数を算出できなかつた。また注目すべきスペ
クトルが接近している場合にも正確な劣化指数を
算出できない。 〔問題点を解決するための手段〕 本発明は、斯かる事情に鑑みてなされたもので
あり異常に起因する振動以外の振動(ノイズ)を
除去し得て、正確な劣化指数を算出し得る回転機
械の診断方法を提供することを目的とする。本発
明は、回転機械における振動を測定し、一過性の
ノイズを除去すべくその測定信号を自己回帰モデ
ル化してパワースペクトルを求め、このパワース
ペクトルの特定周波数における強度とパワースペ
クトルの実効値との比を劣化指数として算出し、
算出された劣化指数から劣化確率を算出すること
を特徴とする。 〔原理〕 本発明方法の原理について以下に説明する。第
1図は、回転機械における振動の検出信号を示
す。今、時刻tにおける振動の大きさをxtとする
と、この信号には、各種因子による振動が重畳し
ていると考えられる。そこでこの信号を、各種振
動の重畳信号と考え、(1)式で示す自己回帰式を設
定する。 xt=a1α1+a2α2+…utMi=1 aiαi+ut ……(1) ai:システムパラメータ αi:時刻tの振動における量子化された振動成分 ut:白色ノイズ(周波数に無関係な定数のパワー
スペクトル密度をもつようなランダム信号) M:システム次数 ここでシステムパラメータ及びシステム次数に
ついて考える。まずシステム次数M=1の場合に
は(1)式は次のように表わされる。 xt=a1α1+ut ……(2) (2)式においてxtを既知(測定値)とすると、 ut=xt−a1α1 ……(2)′ となり、a1α1を推定値と考えればutは誤差を表わ
す。そこで最小2乗法によりa1の最適値を求め
る。つまりut 2の期待値E〔ut 2〕を最小にするa1
値が最適値となる。そしてこの求めた値a1に基づ
いてutの期待値E〔ut〕M=1を演算する。 次にシステム次数M=2の場合について考える
と(1)式は、 xt=a1α1+a2α2+ut ……(3) となる。ここに上述の最小2乗法により求めたa1
の値を代入し、さらに同様の最小2乗法によりa2
を求め、求められた値a1、a2に基づいてutの期待
値E〔utM=2を演算する。そして先に求めたut
期待値E〔utM=1と、このE〔utM=2とを比較す
る。以下同様の手順で期待値E〔utM=iを求め、E
〔utM=i-1とE〔utM=iとの差が所定の微小値以下に
なつた場合におけるiをシステム次数Mとする。
つまりa1α1,a2α2,…,aMαMは夫々原因の異な
る振動成分と考えられ、この振動成分が所定値以
下の微少なものはホワイトノイズとして扱う。従
つて所定の次数Mにて表わされるxtは、時刻tに
おけるノイズを除去した振動を表わす値と考えら
れる。 同様の方法により、所定の時間毎に抽出された
振動信号のノイズを除去する。 このようにして得られるノイズを除去した振動
信号に基づいて、そのパワースペクトルをもとめ
る。パワースペクトルは下記(4)式で表わされる。 但し、 f:周波数 σu2:統計量推定の分散 (4)式によりパワースペクトルが求められるが、
回転機械等に異常があれば、その異常に起因して
パワースペクトルの強度は部分的に大きくなる。
従つてパワースペクトルの強度が部分的に大きく
なつていれば、回転機械等に異常が生じているこ
とが類推されるが、回転機械等の種類、或いは異
常の種類に対応して、異常に起因するパワースペ
クトル強度の突出状態の周波数特性が異なる。そ
こで回転機械の異常の程度を表わす劣化指数とし
て、パワースペクトル強度の全周波数域での実効
値と各異常により規定される特性周波数における
パワースペクトル強度との比率を用いる。 第2図イ〜ホに、回転機械の各異常に起因する
パワースペクトル強度と特性周波数の関係を示
す。第2図イは、回転機械における回転軸がアン
バランスな状態であり、foは回転軸の周波数を示
す。この場合の劣化指数F1は F1=S1/Srms ……(5) 但し、 S1:周波数foにおけるパワースペクトル強度 Srms:パワースペクトルの全周波数域での実効
値 で表わされる。 第2図ロは、回転機械におけるミスアライメン
ト又はベントシヤフトが生じた状態であり、劣化
指数F2は F2=√S2 2+S3 2/Srms ……(6) S2,S3:周波数2fo、3foにおけるパワースペクト
ル強度 で表わされる。 第2図ハは、回転機械にガタが生じている場合
であり、劣化指数F3は F3=S0.5/Srms ……(6) S0.5:周波数1/2foにおけるパワースペクトル強度 で表わされる。 第2図ニは、軸受に異常が生じている場合であ
る。軸受においては、外輪、内輪、転動体夫々に
ついて各別に、この第2図ニに示すようなパワー
スペクトル強度となるが、夫々の周波数特性は異
なる。図におけるKi(i=1〜3)は外輪、内輪、
転動体のいずれかに異常があつた場合におけるそ
の各部に対応する定数であり、K1が外輪異常、
K2が内輪異常、K3が転動体異常の場合を夫々示
している。K1,K2,K3は次のように表わされ
る。 K1=n/2(1−d/Dcosα) ……(7) K2=n/2(1+d/Dcosα) ……(8) K3=D/d{1−(d/D)2cosα} ……(9) 但し、 n:転動体の数 d:転動体の直径 D:転動体のピツチ円の直径 α:転動体の接触角度 外輪、内輪、転動体の各劣化指数は次のように
表わされる。 F4i=√S1 2+S2 2+S3 2/Srms ……(10) F41:外輪の劣化指数 F42:内輪の劣化指数 F43:転動体の劣化指数 S1,S2,S3:周波数Kifo(i=123)2Kifo,
3Kifoにおけるパワースペクトル強度 第2図ホは歯車が劣化した状態におけるパワー
スペクトルの強度と特性周波数の関係を示しfG
歯車のかみ合い周波数であつて、 fG=Z・fo ……(11) Z:歯数 fo:軸の回転数 となる。そして、この歯車の劣化指数F5は F5=√S1 2+S2 2/Srms ……(12) S1,S2:周波数fG,2fGにおける各パワースペク
トル強度 この劣化指数により、異常の状態が認識される
のであるが、さらに異常の程度を評価すべく劣化
確率を求める。一般に、信頼性理論では偶発故障
確率R(t)は、 R(t)=1−e-t ……(13) で求まり、指数分布に従うものとされていて、 劣化確率は劣化指数Fの関数として下記(14)
式にて表わされる。則ち、劣化確率をP(F)、劣
化指数をFとすると、 但し、 Lo:異常が発生していないと考えられる場合
{P(F)=0}の劣化指数の最大値 Mo:寿命{P(F)=1.0}の劣化指数の最大値 Xo:劣化確率が0.5になるときの劣化指数 nx:指数曲線の傾き(異常の種類等により定ま
る) となる。(14)式をグラフにて表わすと、第3図
の如き曲線となる。 本願発明者は、基礎実験、フイールドデータの
確証試験により、第2図イ〜ホに示し、また前記
(5)〜(12)式にて求めた各回転機械等、或いは回
転機械等の各種異常における劣化指数に対する劣
化確率曲線を得た。これを第4〜8図に示す。第
4図は回転軸がアンバランスな状態である場合に
おける劣化指数と劣化確率との関係を示し、第5
図は回転機械のミスアライメント又はベントシヤ
フト状態である場合における劣化指数と劣化確率
との関係を示し、第6図は回転機械にガタが生じ
ている場合における劣化指数と劣化確率との関係
を示している。第7図イ〜ハは軸受に異常が生じ
た場合を示し、第7図イは軸受の外輪における異
常が生じている場合、第7図ロは軸受の内輪に異
常が生じている場合、第7図ハは軸受の転動体に
異常が生じている場合の劣化指数に対する劣化確
率を夫々示している。第8図は歯車において異常
が生じた場合の劣化指数に対する劣化確率を示し
ている。 従つて、前記(5)〜(12)式にて劣化指数を求め
ると第4図〜第8図のグラフにより劣化確率が求
まり、各回転機械における具体的な異常の程度が
把握できることになる。 〔実施例〕 第9図は本発明方法の実施に使用される装置の
模式的ブロツク図である。図において1はモータ
であり、該モータ1の出力軸はカツプリング2に
て軸5に連結されている。該軸5は両端を軸受
3,3にて夫々回転自在に支持されており、軸5
には油圧シリンダ6にて荷重が負荷されている。 一方の軸受3には、振動ピツクアツプ7が取付
けられており、軸受3の振動を捉えて振動計8に
所定信号を出力する。振動計8の出力はA/D変
換器9を介して演算処理部10に与えられてお
り、演算処理部10は前述した如くA/D変換器
9の出力に基づいて、所定の時間毎に軸受3の振
動を抽出し、各時間における振動を量子化して振
動に重畳されたノイズを除去する。そして各時間
におけるノイズを除去した振動に基づいてパワー
スペクトルを演算して夫々の劣化指数を算出す
る。さらに予め設定された劣化指数と劣化確率と
の関係から、劣化確率を演算する。演算処理部1
0の演算結果は、表示・印字部11にて表示・印
字される。 この装置を用いて正常な軸受を診断した場合に
おける自己回帰モデルにより得られたパワースペ
クトルを第10図に示す。また、第11図に外輪
に人工欠陥を付与した軸受の自己回帰モデルによ
り得られたパワースペクトルを示す。 さらに正常、外輪異常の各軸受の劣化指数、及
び劣化指数から求められた劣化確率を夫々第1表
に示す。第1表より明らかなように、外輪の劣化
確率が100%となり、外輪に異常が生じているこ
とが明らかになる。 なお、第12図に、正常な軸受の振動を高速フ
ーリエ変換した結果を、また第13図に外輪に人
工欠陥を付与した軸受の振動を高速フーリエ変換
した結果を夫々に示す。
[Industrial Application Field] The present invention relates to a method for diagnosing abnormal conditions in rotating machines such as reducers, motors, and blowers, or rotating machine elements such as bearings and gears. [Prior Art] In rotating machines such as motors and blowers, or rotating machine elements such as rolling bearings and gears, wear and damage due to rotation, damage due to poor lubrication, and damage due to poor assembly occur. For this reason,
It becomes necessary to detect and deal with damage caused to rotating machinery and the like at an early stage. Diagnostic methods for abnormalities in rotating machinery include wear,
Vibration methods that capture vibrations caused by abnormalities such as damage are common. Conventional vibration methods measure the vibrations of rotating machinery, etc., and perform fast Fourier transform on the vibrations to convert the vibrations, which are irregular functions expressed in the time domain, into functions in the frequency domain, and calculate their power spectrum. was determined, and a deterioration index was calculated from the determined power spectrum to determine abnormal conditions in rotating machinery, etc. [Problem to be solved by the invention] Vibrations in rotating machines, etc. include vibrations (noise) other than vibrations caused by abnormalities such as wear and damage, especially transient ones, so conventional vibrations The method could not completely remove these noises, and an accurate deterioration index could not be calculated. Furthermore, it is not possible to accurately calculate the deterioration index even when the spectra of interest are close to each other. [Means for solving the problem] The present invention has been made in view of the above circumstances, and can remove vibrations (noise) other than vibrations caused by abnormalities, and can calculate accurate deterioration index. The purpose is to provide a diagnostic method for rotating machinery. The present invention measures vibrations in a rotating machine, calculates a power spectrum by applying an autoregressive model to the measured signal to remove transient noise, and calculates the intensity at a specific frequency of this power spectrum and the effective value of the power spectrum. The ratio of is calculated as the deterioration index,
The method is characterized in that a deterioration probability is calculated from the calculated deterioration index. [Principle] The principle of the method of the present invention will be explained below. FIG. 1 shows a detection signal of vibration in a rotating machine. Now, if the magnitude of vibration at time t is xt , it is considered that vibrations due to various factors are superimposed on this signal. Therefore, considering this signal as a superimposed signal of various vibrations, an autoregressive equation shown in equation (1) is set. x t = a 1 α 1 + a 2 α 2 +…u t = Mi=1 a i α i +u t …(1) a i : System parameter α i : Quantized vibration in the vibration at time t Component u t : White noise (a random signal having a constant power spectral density independent of frequency) M : System order Here, consider the system parameters and system order. First, when the system order M=1, equation (1) can be expressed as follows. x t = a 1 α 1 + u t ……(2) In equation (2), if x t is known (measured value), then u t = x t −a 1 α 1 ……(2)′, and a 1 If α 1 is considered as an estimated value, u t represents the error. Therefore, the optimum value of a 1 is determined by the method of least squares. In other words, the value of a 1 that minimizes the expected value E[u t 2 ] of u t 2 is the optimal value. Then, based on the obtained value a1 , the expected value E[u t ]M=1 of ut is calculated. Next, considering the case where the system order M=2, equation (1) becomes x t =a 1 α 1 +a 2 α 2 + ut (3). Here, a 1 obtained by the above least squares method
Substituting the value of a 2
The expected value E[ ut ] M=2 of u t is calculated based on the obtained values a 1 and a 2 . Then, the previously obtained expected value E[u t ] M = 1 of u t and this E[u t ] M = 2 are compared. Below, use the same procedure to find the expected value E [u t ] M=i , and
Let i be the system order M when the difference between [u t ] M=i-1 and E[u t ] M=i becomes a predetermined minimum value or less.
In other words, a 1 α 1 , a 2 α 2 , . . . , a M α M are considered to be vibration components with different causes, and if these vibration components are minute and are less than a predetermined value, they are treated as white noise. Therefore, x t expressed by a predetermined order M is considered to be a value representing the vibration from which noise is removed at time t. A similar method is used to remove noise from vibration signals extracted at predetermined time intervals. Based on the vibration signal obtained in this way from which noise has been removed, its power spectrum is determined. The power spectrum is expressed by the following equation (4). However, f: Frequency σu 2 : Variance of statistical estimation The power spectrum can be obtained from equation (4), but
If there is an abnormality in a rotating machine or the like, the intensity of the power spectrum will partially increase due to the abnormality.
Therefore, if the intensity of the power spectrum is partially large, it can be inferred that an abnormality has occurred in a rotating machine, etc., but depending on the type of rotating machine, etc. or the type of abnormality, it can be assumed that the cause is due to an abnormality. The frequency characteristics of the prominent state of the power spectrum intensity are different. Therefore, as a deterioration index representing the degree of abnormality in a rotating machine, the ratio between the effective value of the power spectrum intensity in the entire frequency range and the power spectrum intensity at the characteristic frequency defined by each abnormality is used. FIG. 2 A to E show the relationship between the power spectrum intensity and the characteristic frequency caused by each abnormality in the rotating machine. Figure 2A shows the state in which the rotating shaft of a rotating machine is unbalanced, and fo indicates the frequency of the rotating shaft. The deterioration index F 1 in this case is F 1 =S 1 /Srms (5) where, S 1 : power spectrum intensity at frequency fo Srms : expressed as an effective value in the entire frequency range of the power spectrum. Figure 2 (b) shows a state in which misalignment or bent shaft occurs in a rotating machine, and the deterioration index F 2 is F 2 =√S 2 2 + S 3 2 /Srms ……(6) S 2 , S 3 : Frequency It is expressed as the power spectrum intensity at 2fo and 3fo. FIG. 2C shows a case where there is play in the rotating machine, and the deterioration index F 3 is expressed by the power spectrum intensity at frequency 1 / 2fo. FIG. 2D shows a case where an abnormality has occurred in the bearing. In a bearing, the outer ring, inner ring, and rolling elements each have a power spectrum intensity as shown in FIG. 2D, but the frequency characteristics of each are different. K i (i=1 to 3) in the figure is the outer ring, the inner ring,
It is a constant corresponding to each part when there is an abnormality in any of the rolling elements, K 1 is the outer ring abnormality,
K 2 shows the inner ring abnormality, and K 3 shows the rolling element abnormality. K 1 , K 2 , and K 3 are expressed as follows. K 1 =n/2(1-d/Dcosα) ……(7) K 2 =n/2(1+d/Dcosα) ……(8) K 3 =D/d{1-(d/D) 2 cosα } ...(9) However, n: Number of rolling elements d: Diameter of the rolling element D: Diameter of pitch circle of the rolling element α: Contact angle of the rolling element Each deterioration index of the outer ring, inner ring, and rolling element is as follows. is expressed in F 4i =√S 1 2 +S 2 2 +S 3 2 /Srms...(10) F 41 : Outer ring deterioration index F 42 : Inner ring deterioration index F 43 : Rolling element deterioration index S 1 , S 2 , S 3 :Frequency Kifo (i= 1 , 2 , 3 )2Kifo,
3 Power spectrum intensity in Kifo Figure 2 E shows the relationship between the power spectrum intensity and characteristic frequency when the gear is in a deteriorated state, where f G is the meshing frequency of the gear, and f G = Z・fo......(11) Z : Number of teeth fo: Number of rotations of the shaft. Then, the deterioration index F 5 of this gear is F 5 =√S 1 2 + S 2 2 /Srms ... (12) S 1 , S 2 : Each power spectrum intensity at frequency f G , 2f G This deterioration index causes abnormality. The state is recognized, but the probability of deterioration is determined to further evaluate the degree of abnormality. In general, in reliability theory, the random failure probability R(t) is determined as R(t) = 1-e -t ...(13) and is said to follow an exponential distribution, and the deterioration probability is determined by the deterioration index F. Below as a function (14)
It is expressed by the formula. In other words, if the probability of deterioration is P(F) and the deterioration index is F, then However, Lo: Maximum value of deterioration index when no abnormality is considered to occur {P(F)=0} Mo: Maximum value of deterioration index during life {P(F)=1.0} Xo: Deterioration probability The deterioration index nx when it becomes 0.5 is the slope of the exponential curve (determined by the type of abnormality, etc.). When equation (14) is expressed graphically, it becomes a curve as shown in FIG. Through basic experiments and confirmatory tests of field data, the inventor of the present application has obtained the results shown in FIG.
Deterioration probability curves were obtained for each rotary machine or the deterioration index for various abnormalities in the rotary machine, etc., obtained using equations (5) to (12). This is shown in Figures 4-8. Figure 4 shows the relationship between the deterioration index and the deterioration probability when the rotation axis is unbalanced.
The figure shows the relationship between the deterioration index and the probability of deterioration when the rotating machine is in a misalignment or bent shaft state, and Figure 6 shows the relationship between the deterioration index and the probability of deterioration when there is play in the rotating machine. ing. Figures 7A to 7C show cases where an abnormality occurs in the bearing. Figure 7A shows a case where an abnormality occurs in the outer ring of the bearing, and Figure 7B shows a case where an abnormality occurs in the inner ring of the bearing. Figure 7C shows the deterioration probability relative to the deterioration index when an abnormality occurs in the rolling elements of the bearing. FIG. 8 shows the deterioration probability relative to the deterioration index when an abnormality occurs in the gear. Therefore, when the deterioration index is determined using the above equations (5) to (12), the deterioration probability is determined from the graphs shown in FIGS. 4 to 8, and the specific degree of abnormality in each rotating machine can be grasped. [Example] FIG. 9 is a schematic block diagram of an apparatus used to carry out the method of the present invention. In the figure, 1 is a motor, and the output shaft of the motor 1 is connected to a shaft 5 through a coupling 2. The shaft 5 is rotatably supported at both ends by bearings 3, 3, respectively.
A load is applied to the hydraulic cylinder 6. A vibration pickup 7 is attached to one of the bearings 3, which captures vibrations of the bearing 3 and outputs a predetermined signal to a vibration meter 8. The output of the vibrometer 8 is given to the arithmetic processing section 10 via the A/D converter 9, and the arithmetic processing section 10, as mentioned above, performs vibrations at predetermined intervals based on the output of the A/D converter 9. The vibration of the bearing 3 is extracted, the vibration at each time is quantized, and noise superimposed on the vibration is removed. Then, a power spectrum is calculated based on the vibration from which noise has been removed at each time, and each deterioration index is calculated. Furthermore, the deterioration probability is calculated from the relationship between the preset deterioration index and the deterioration probability. Arithmetic processing unit 1
The calculation result of 0 is displayed and printed on the display/print section 11. FIG. 10 shows a power spectrum obtained by an autoregressive model when a normal bearing is diagnosed using this device. Moreover, FIG. 11 shows a power spectrum obtained by an autoregressive model of a bearing with an artificial defect added to the outer ring. Furthermore, Table 1 shows the deterioration index of each bearing, normal and abnormal, and the deterioration probability determined from the deterioration index. As is clear from Table 1, the probability of deterioration of the outer ring is 100%, and it becomes clear that an abnormality has occurred in the outer ring. Note that FIG. 12 shows the results of fast Fourier transform of the vibrations of a normal bearing, and FIG. 13 shows the results of fast Fourier transform of the vibrations of a bearing with an artificial defect on the outer ring.

〔効果〕〔effect〕

本発明によれば、回転機械の異常の種類、程度
をノイズ等の影響を受けることなく、明確に捉え
ることができ、回転機械等の診断を高精度に行え
る。
According to the present invention, the type and degree of abnormality in a rotating machine can be clearly grasped without being affected by noise, etc., and the rotating machine, etc. can be diagnosed with high accuracy.

【図面の簡単な説明】[Brief explanation of drawings]

第1図は本発明方法の説明のためのグラフ、第
2図イ〜ホは、劣化指数算出方法説明のためのグ
ラフ、第3図〜第8図は劣化指数と劣化確率との
関係を示すグラフ、第9図は本発明方法の実施に
使用する装置の模式的ブロツク図、第10図、第
11図は軸受の振動を本発明方法における自己回
帰モデル化したグラフ、第12図、第13図は、
軸受の振動を従来方法における高速フーリエ変換
したグラフである。 1……モータ、2……カツプリング、3……軸
受、5……軸、7……振動ピツクアツプ。
Fig. 1 is a graph for explaining the method of the present invention, Fig. 2 I to E are graphs for explaining the deterioration index calculation method, and Figs. 3 to 8 show the relationship between the deterioration index and the probability of deterioration. Graphs, FIG. 9 is a schematic block diagram of the apparatus used to carry out the method of the present invention, FIGS. 10 and 11 are graphs showing autoregressive modeling of bearing vibration in the method of the present invention, and FIGS. 12 and 13. The diagram is
It is a graph obtained by fast Fourier transform of bearing vibration using a conventional method. 1...Motor, 2...Coupling, 3...Bearing, 5...Shaft, 7...Vibration pick-up.

Claims (1)

【特許請求の範囲】[Claims] 1 回転機械における振動を測定し、一過性のノ
イズを除去すべくその測定信号を自己回帰モデル
化してパワースペクトルを求め、このパワースペ
クトルの特定周波数における強度とパワースペク
トルの実効値との比を劣化指数として算出し、算
出された劣化指数から劣化確率を算出することを
特徴とする回転機械の診断方法。
1. Measure the vibration in a rotating machine, create a power spectrum by modeling the measured signal into an autoregressive model to remove transient noise, and calculate the ratio of the intensity at a specific frequency of this power spectrum to the effective value of the power spectrum. A method for diagnosing a rotating machine, characterized by calculating a deterioration index and calculating a deterioration probability from the calculated deterioration index.
JP59236928A 1984-11-09 1984-11-09 Diagnosing method of rotary machine Granted JPS61114134A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP59236928A JPS61114134A (en) 1984-11-09 1984-11-09 Diagnosing method of rotary machine

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP59236928A JPS61114134A (en) 1984-11-09 1984-11-09 Diagnosing method of rotary machine

Publications (2)

Publication Number Publication Date
JPS61114134A JPS61114134A (en) 1986-05-31
JPH0422456B2 true JPH0422456B2 (en) 1992-04-17

Family

ID=17007826

Family Applications (1)

Application Number Title Priority Date Filing Date
JP59236928A Granted JPS61114134A (en) 1984-11-09 1984-11-09 Diagnosing method of rotary machine

Country Status (1)

Country Link
JP (1) JPS61114134A (en)

Families Citing this family (5)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH05187971A (en) * 1992-01-17 1993-07-27 Hitachi Electron Service Co Ltd Acoustically diagnosing device for air-cooling fan
JP3652673B2 (en) * 2002-08-06 2005-05-25 三菱電機株式会社 Vibration characteristic evaluation method and apparatus
CN113454363B (en) * 2019-02-22 2024-07-26 株式会社日本制钢所 Abnormality detection system and abnormality detection method
KR102648646B1 (en) * 2023-05-23 2024-03-15 호서대학교 산학협력단 Apparatus for predicting failure based on artificial intelligence and method therefor
KR102649659B1 (en) * 2023-05-23 2024-03-19 호서대학교 산학협력단 Apparatus for training artificial intelligence model for failure prediction and method therefor

Also Published As

Publication number Publication date
JPS61114134A (en) 1986-05-31

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